Theodoros K Karamanos1, Clare L Pashley1, Arnout P Kalverda1, Gary S Thompson1, Maxim Mayzel2, Vladislav Y Orekhov2,3, Sheena E Radford1. 1. Astbury Centre for Structural Molecular Biology and School of Molecular and Cellular Biology, University of Leeds , Leeds LS2 9JT, U.K. 2. The Swedish NMR Centre, University of Gothenburg , Box 465, 40530 Göteborg, Sweden. 3. Department of Chemistry and Molecular Biology, University of Gothenburg , Box 465, 40530 Göteborg, Sweden.
Abstract
The balance between protein folding and misfolding is a crucial determinant of amyloid assembly. Transient intermediates that are sparsely populated during protein folding have been identified as key players in amyloid aggregation. However, due to their ephemeral nature, structural characterization of these species remains challenging. Here, using the power of nonuniformly sampled NMR methods we investigate the folding pathway of amyloidogenic and nonamyloidogenic variants of β2-microglobulin (β2m) in atomic detail. Despite folding via common intermediate states, we show that the decreased population of the aggregation-prone ITrans state and population of a less stable, more dynamic species ablate amyloid formation by increasing the energy barrier for amyloid assembly. The results show that subtle changes in conformational dynamics can have a dramatic effect in determining whether a protein is amyloidogenic, without perturbation of the mechanism of protein folding.
The balance between protein folding and misfolding is a crucial determinant of amyloid assembly. Transient intermediates that are sparsely populated during protein folding have been identified as key players in amyloid aggregation. However, due to their ephemeral nature, structural characterization of these species remains challenging. Here, using the power of nonuniformly sampled NMR methods we investigate the folding pathway of amyloidogenic and nonamyloidogenic variants of β2-microglobulin (β2m) in atomic detail. Despite folding via common intermediate states, we show that the decreased population of the aggregation-prone ITrans state and population of a less stable, more dynamic species ablate amyloid formation by increasing the energy barrier for amyloid assembly. The results show that subtle changes in conformational dynamics can have a dramatic effect in determining whether a protein is amyloidogenic, without perturbation of the mechanism of protein folding.
Protein unfolding is
commonly associated with amyloid formation.
This view is supported by the large number of intrinsically unfolded
proteins that are the causative agents of amyloid diseases, such as
α-synuclein, amyloid-β peptide (Aβ), and amylin.[1−3] In terms of folded protein precursors, a link between local or global
unfolding and the onset of aggregation has been documented.[4] Indeed, decreased native state stability and
a reduction in co-operativity have been linked with enhanced amyloidogenicity
of several proteins, including human lysozyme,[5] transthyretin,[6] prion protein,[7] superoxide dismutase (SOD),[8] and β2-microglobulin (β2m).[9,10] These findings have guided theoretical approaches
to predict aggregation-prone regions of folded proteins by combining
the intrinsic propensity of a protein sequence to self-assemble with
its probability to become exposed (e.g., by increased predicted hydrogen-exchange
rates).[11,12] Along similar lines, strategies to stabilize
native-like conformations by the use of small molecules,[13,14] aptamers,[15] molecular chaperones[16,17] or via other protein–protein interactions[18,19] all reduce amyloid formation. However, a quantitative link between
the conformational properties and dynamics of individual partially
folded species and amyloid propensity remains elusive, in part because
of difficulties in identifying and characterizing amyloid intermediates
in atomic detail. In addition, the complexity of the energy landscape
of proteins, which involves many potentially amyloidogenic species,
exacerbates the intricacy of the system.In this study we investigate
the structural, kinetic, and thermodynamic
properties of sparsely populated intermediates of human and murine
β2m (hβ2m, mβ2m,
respectively) and link their properties to the known, very different
amyloid propensities of these proteins.[20] Hβ2m forms amyloid fibrils in the joints of patients
undergoing hemodialysis, in a pathological condition known as dialysis-related
amyloidosis.[21,22] Previous studies have examined
the link between the folding pathway of β2m and its
aggregation propensity. These studies showed that hβ2m does not aggregate at neutral pH unless additives such as Cu2+,[23] trifluoroethanol (TFE),[24] or other cosolvents,[25,26] which partially unfold the protein, are added. As hβ2m contains a thermodynamically unfavorable cis prolyl-peptide
bond at position 32, protein folding involves a slow folding phase
which is attributed to trans–cis proline isomerization of this bond.[9,27] A native-like
intermediate containing a trans-Pro 32 (IT) accumulates during folding of hβ2m, which can
be trapped by removal of the N-terminal six residues of the protein,
to create the variant ΔN6.[28,29] At neutral
pH, the concentration of IT correlates directly with the
rate of amyloid formation of hβ2m,[9] suggesting that formation of this on-pathway native-like
folding intermediate is a key determinant of amyloid formation. This
supposition is confirmed by the ability of ΔN6 to aggregate
readily at pH 6.2.[28] On the other hand,
mβ2m, despite being 70% identical in sequence to
hβ2m and also containing a cis-X
Pro 32 bond, does not form amyloid fibrils at neutral pH, or even
when unfolded under acidic conditions (unless high concentrations
of salt are added) (Figure A and 1B).[19,30] The basis of such dramatically different amyloid propensities despite
the sequence and structural similarities of these two proteins remained
unclear.
Figure 1
Structure and amyloidogenicity of mβ2m. (A) The
NMR structure of monomeric hβ2m (gray-2XKS[28]) overlaid with the crystal structure of mβ2m bound to the MHC-I complex (green-1LK2[38]) or with the solution structure of ΔN6 (red-2XKU[28]). (B) Aggregation assay of 80 μM hβ2m (gray), mβ2m (green), or ΔN6 (red)
in 10 mM sodium phosphate buffer, pH 6.2 (three replicates for each
protein). Negative stain electron micrographs, color-coded with the
same scheme, are shown on the right (scale bar = 500 nm). (C) The 1H–15N HSQC spectrum of mβ2m in the same buffer as (B). (D) Correlation between experimental
RDCs measured for mβ2m in 10 mg/mL phage PF1 and
those back-calculated from the crystal structure 1LK2[38] (R2 = 0.85).
Structure and amyloidogenicity of mβ2m. (A) The
NMR structure of monomeric hβ2m (gray-2XKS[28]) overlaid with the crystal structure of mβ2m bound to the MHC-I complex (green-1LK2[38]) or with the solution structure of ΔN6 (red-2XKU[28]). (B) Aggregation assay of 80 μM hβ2m (gray), mβ2m (green), or ΔN6 (red)
in 10 mM sodium phosphate buffer, pH 6.2 (three replicates for each
protein). Negative stain electron micrographs, color-coded with the
same scheme, are shown on the right (scale bar = 500 nm). (C) The 1H–15N HSQC spectrum of mβ2m in the same buffer as (B). (D) Correlation between experimental
RDCs measured for mβ2m in 10 mg/mL phage PF1 and
those back-calculated from the crystal structure 1LK2[38] (R2 = 0.85).Here, we set out to investigate the molecular origins
of the reduced
amyloidogenicity of mβ2m. We characterize the stability,
structure, and dynamics of the native protein and show that despite
its inability to form amyloid, mβ2m is kinetically
and thermodynamically less stable than its human counterpart. The
folding pathway of mβ2m is then explored using real-time
NMR, taking advantage of the power of nonuniformly sampling (NUS)
methods to reveal detailed information on the energy landscape of
mβ2m folding. Combined with other biophysical methods,
we show that while mβ2m also folds through an IT state, this species is relatively more flexible than its
hβ2m counterpart and in conformational exchange with
other, less-structured non-native states.The molten globule-like
characteristics of the mβ2m folding intermediate
reduce the lifetime of the structured, well-folded
IT state, which now represents only a minor substate in
the structural ensemble. Our findings confirm the vital role of IT (and hence a highly structured, yet non-native species) in
determining the aggregation of β2m. Moreover, the
results highlight the importance of defining the energy landscape
of amyloidogenic proteins in detail to allow prediction of their amyloid
propensity. The findings presented also suggest that targeting a defined
non-native species should be a successful means of controlling the
fate of assembly of β2m and, in principle, that of
other amyloidogenic proteins which aggregate via a specific, non-native
precursor.
Methods
Protein Preparation
The pINK plasmid containing the
hβ2m, mβ2m, or ΔN6 gene was
transformed into E. coli cells of the BL21 DE3 plysS-
strain. Starter cultures were generated by inoculating 100 mL of LB
medium with cells containing the relevant gene and 50 μg/mL
carbenicilin and 50 μg/mL chloramphenicol and incubating overnight
at 37 °C, 200 rpm. 2 L flasks containing 1 L of LB or HDMI (1
g/L 15N-NH4Cl, 2 g/L 13C-glucose)
medium were inoculated with 10 mL of starter culture. Cells were incubated
at 37 °C, 200 rpm until they reached an OD600 of ∼0.6
and then the expression of β2m was induced by the
addition of isopropyl β-d-1-thiogalactopyranoside (IPTG-final
concentration of 1 mM). Expression was allowed to continue overnight
at 37 °C, and cells were harvested next morning using a Heraus
continual action centrifuge performing at 15 000 rpm. The cell
pellet containing β2m as inclusion bodies was chemically
lysed by the addition of 50–100 mL of lysis buffer (100 μg/mL
lysozyme, 50 μg/mL DNase I, 50 μg/mL phenylmethylesulfonyl
fluoride (PMSF), 10 mM Tris-HCl pH 8.0). Further cell disruption was
performed using a constant cell disrupter system (Constantsystems)
at a high pressure of 20.0 kpsi. Inclusion bodies were separated using
centrifugation (15 000 rpm using a Sorvall SS34 rotor) in a
Beckman centrifuge for 40 min at 4 °C, and the inclusion body
pellet was washed with 10 mM Tris-HCl pH 8.0 buffer four times. Finally,
β2m was solubilized in 10–20 mM Tris-HCl pH
8.0 (hβ2m, ΔN6) or 10–20 mM Tris-HCl
pH 8.5 (mβ2m) containing 8 M urea (MP biomedicals)
and refolded by dialysis (3000 MW cutoff) against 2–5 L of
the same buffer but lacking urea. The refolded protein was centrifuged
for 30 min at 15000 rpm (Sorvall SS34 rotor) to pellet insoluble material,
and the supernatant was loaded on a Q-Sepharose (GE Healthcare) column
already equilibrated with 2 column volumes of 20 mM Tris-HCl pH 8.0
(hβ2m, ΔN6) or 20 mM Tris-HCl pH 8.5 (mβ2m) for anion exchange purification. Bound protein was eluted
with a gradient of 0–400 mM NaCl (in the same buffer) over
800 mL and was freeze-dried after dialysis in dH2O or concentrated
using 3000 MW cutoff centricons (Avanti LTD). Freeze-dried protein
was resuspended in 10 mM sodium phosphate buffer pH 7.0 (hβ2m, ΔN6) and 10 mM sodium phosphate buffer pH 8.2 (mβ2m) filtered through 0.2 μm filters (Fisher Scientific)
and gel-filtered using a HiLoad Superdex-75 Prep column (Amersham
Biosciences), calibrated with a standard gel filtration calibration
kit (GE Healthcare). The monomer peak was collected, concentrated,
aliquoted, and stored at −80 °C or freeze-dried.
NMR Spectroscopy
Assignments of the backbone atoms
of mβ2m were obtained using samples of 500 or 750
μM uniformly labeled (15N, 13C) protein
in 10 mM sodium phosphate buffer pH 6.2, 83.3 mM NaCl, 0.02% (w/v)
NaN3, and 10% (v/v) D2O. Three-dimensional (3D)
NMR experiments were recorded at 25 °C using Varian Inova spectrometers
(Agilent) operating at proton frequencies of 500 MHz (HNCA, HNCO,
CBCA(CO)NH, HN(CA)CO) and 750 MHz (HNCACB), equipped with a room temperature
or cryogenic probe, respectively. Samples for H/D exchange experiments
were prepared in 10 mM sodium phosphate buffer pH 6.2 and then freeze-dried.
Freeze-dried protein was dissolved in 100% (v/v) D2O containing
83.3 mM NaCl and placed into the NMR tube after manual mixing. The
loss of intensity of amide proton resonances was then monitored by
SOFAST 1H–15N HSQC[31] spectra (5–10 min each) at 25 °C. Residual
dipolar coupling (RDC) experiments (J modulated series) were carried
out using a sample of 200 μM 15N-mβ2m in 10 mM sodium phosphate pH 8.2 and aligned in 11 mg/mL bacteriophage
PF1 (Asla Scientific). RDC data were back-calculated from crystal
structures using PALES.[32] For relaxation
experiments, a sample of 80 μM 15N-mβ2m was prepared in 10 mM sodium phosphate buffer at pH 6.2 with 10%
(v/v) D2O, 0.02% (w/v) NaN3, 83.3 mM NaCl. T2 experiments were perfomed with 2048 and 128 complex points
in the direct and indirect dimension using 18.8, 37.7, 56. 6, 75.5,
94.4, 113.2, 132,1, 151.0 ms as relaxation delays. The relaxation
delays for the T1 experiments were 0.0.16, 0.32, 0.48,
0.64, 0.80, 0.96, 1.12, 1.44 s. For 1H–15N NOE cross-relaxation experiments saturation of amide protons was
achieved with a train of 120° pulses for 3.5 s prior to the experiment.
All relaxation and RDC experiments were performed at 25 °C, using
a 600 MHz Varian Inova spectrometer equipped with a room tempreature
probe. Direct carbon detection experiments were performed using a
sample of 13C, 15N mβ2m at
1.3 mM on a 950 MHz Bruker spectrometer equipped with a cryogenic
TCI probe (1024 and 160 complex points in the direct and indirect
dimensions).For real-time refolding experiments two refolding
protocols were followed: (1) protein samples were made in 10 mM sodium
phosphate buffer pH 6.2 and freeze-dried. Unfolding was performed
by dissolving the freeze-dried protein (2–3 mg) in 30–60
μL of the same buffer containing 8 M urea at 37 °C for
1 h, and the protein was then refolded by rapid 10-fold dilution in
10 mM sodium phosphate pH 6.2, 10% (v/v) D2O, and 0.02%
(w/v) NaN3; (2) protein samples were made in 250 μL
of 10 mM sodium phosphate and 10% (v/v) D2O, and the pH
was adjusted to 2.0 (or pH 3.6) using Tris-HCl. Refolding was then
initiated by addition of 50 μL of 300 mM sodium phosphate buffer,
pH 7.2 (final pH 6.1–6.3). Both refolding protocols were found
to give rise to similar spectra of the intermediate species. This
observation demonstrates that the increased flexibility of the murine
intermediate (see Results) is not the result
of the residual 0.8 M urea present at the end of the first refolding
protocol. The refolding from IT to native hβ2m was monitored by a series of SOFAST 1H–15N HSQC spectra[31,33] at 25 °C, with
80 increments in the indirect dimension, two scans per increment and
512 complex points, resulting in a total acquisition time of 45 s.To assign the I1 state of mβ2m, refolding
was monitored by continuous acquisition of NUS NMR spectra. 3D HNCO+
and HNCA+[34] with a total acquisition time
of ca. 17 h for each spectrum and 2D 1H–15N BEST-TROSY[35] were collected on separate
samples (800 MHz Bruker AVANCE III HD spectrometer with 3 mm TCI cryoprobe).
2D 1H–15N BEST-TROSY, having the highest
sensitivity, was chosen as a reference spectrum to guide 3D spectra
multidimensional decomposition (MDD) coprocessing with a sliding time
frame window, resulting in a temporal resolution of a few minutes[36] (see Supplementary Methods).To aid assignment of the real-time spectra, two samples
were prepared
in which the early intermediate of mβ2m was highly
populated. The first consisted of 600 μM of uniformly labeled 13C, 15N mβ2m in 10 mM sodium phosphate
and 10 mM sodium acetate pH 3.6, and the second consisted of 250 μM
of uniformly labeled 13C, 15N mβ2m in 10 mM sodium phosphate pH 6.2 with 1 M urea added. Both samples
gave rise to HNCA spectra that closely resembled the real-time HNCA
spectrum of the early intermediate of mβ2m. Additional
3D spectra were performed using these samples including HNCA, HNCO,
and CBCACONH utilizing a 600 MHz Varian Inova spectrometer equipped
with a room tempreature probe. TALOS+[37] was used to predict the backbone order parameter (S2).
TALOS+ uses H, NH, Co, Cα, and Cβ backbone chemical shifts
to calculate the random coil chemical shift index which is then converted
to backbone S2. Aggregation assays performed on these samples
confirmed that the early folding intermediate of mβ2m is not aggregation-prone.
Aggregation Assays
Samples containing
60 μM protein
in 10 mM sodium phosphate buffer, pH 6.2, or 10 mM sodium phosphate,
with 10 mM sodium acetate pH 3.6, or in 10 mM sodium phosphate buffer,
pH 6.2, with 1 M urea, with the appropriate amount of NaCl added to
give a total ionic strength of 100 mM), 0.02% (w/v) NaN3 and 10 μM Thioflavin T (ThT) were incubated at 37 °C
in sealed 96 well plates (Thermo Scientific) with agitation at 600
rpm. Fluorescence was monitored at 480 ± 10 nm after excitation
at 440 ± 10 nm using a FLUOROstar Optima microplate reader (BMG
Labtech).
Equilibrium Unfolding
Urea stock solutions containing
75 mM sodium phosphate buffer, pH 6.2, and either no urea or 10.5
M urea were made, and the exact concentration of urea was determined
using the measured refractive index (Ceti refractometer). The stock
solutions were used to make samples of protein containing 0–10
M urea in 0.2 M increments, with a final protein concentration of
0.2 mg/mL. Samples were incubated at 25 °C for 12 h before analysis
using tryptophan fluorescence. Fluorescence was excited at 295 nm,
and the emission was monitored at 340 nm using a Photon Technology
International QM-1 spectrofluorimeter (PTI). The data were then globally
fit to a two-state model:where ΔGoUF (kJ mol–1) is the equilibrium stability, MUF is the equilibrium m-value, a and c represent the denaturant-dependence
of the folded and unfolded signal intensities, respectively, and b
and d are the signal intensities of the folded and unfolded states,
respectively, in the absence of denaturant.
Electron Microscopy (EM)
Carbon coated copper grids
were prepared by the application of a thin layer of Formvar with an
overlay of carbon. Samples were centrifuged (14 000g, 10 min), and the pellets were resuspended in fresh 10
mM sodium phosphate buffer, pH 6.2, diluted to a final protein concentration
of 12 μM with deionized water and then applied to the grid in
a dropwise fashion. The grid was then carefully dried with filter
paper before it was negatively stained by the addition of 18 μL
of 2% (w/v) uranyl acetate. Micrographs were recorded on a Philips
CM10 or a JEOL JEM-1400 electron microscope.
Stopped Flow Experiments
Experiments were performed
using an Applied-Photophysics SX1.8MV stopped-flow fluorimeter. The
temperature was held constant at 37 °C (±0.1 °C) using
a Neslab circulating water bath system. Experiments were performed
in buffered solutions containing 10 mM sodium phosphate (pH 6.2) and
83.3 mM sodium chloride with or without 0.4 M sodium sulfate. Refolding
experiments were performed by 1:10 dilution of 80 μM protein
in buffer containing 8 M urea, into buffered solutions with final
urea concentrations in the range 0.75–8.0 M. The final urea
concentration ranged from 3.0 to 8.0 M for unfolding experiments.
To obtain refolding data at 0 M urea, a pH jump was performed by a
1:10 dilution of 80 μM protein in 10 mM phosphate (pH 2.5) into
80 mM sodium phosphate (pH 6.2). Data were normalized to the signal
of the folded and unfolded protein in 0 and 8 M urea, respectively.
At each urea concentration at least seven kinetic traces were obtained,
averaged, and fitted to a single exponential function using the manufacturer’s
software. ΔGoUI1 was
determined by plotting the fluorescence at the end point of a 20 s
kinetic trace of folding against urea concentration and by plotting
the fluorescence of the unfolded state against urea concentration
(in the latter case, the values at low urea concentration were obtained
by linear extrapolation from the values at high urea concentration).
The fluorescence of the IT state decreased with increasing
urea concentration until it approached the fluorescence of the unfolded
state. To estimate ΔGoUI1 at 0 M urea, data were also recorded in the presence of 0.4 M Na2SO4 and the data in 0 and 0.4 M Na2SO4 were fitted globally to eq .
Results
The native state of mβ2m is thermodynamically
unstable
As well as being 70% identical in sequence, mβ2m and hβ2m/ΔN6 have similar structures
(backbone RMSD ≈ 1.5 Å) (Figure A). However, only ΔN6 is able to aggregate
into amyloid fibrils at pH 6.2 as monitored by the increase in ThT
fluorescence and by negative stain EM (Figure B), in agreement with previous studies.[19] To enable NMR studies of mβ2m, chemical shift assignments were obtained for the native monomeric
protein using a range of 3D NMR experiments (BMRB 19772) (85% of backbone
atoms were assigned; see Methods). The 1H–15N HSQC spectrum of native mβ2m at pH 6.2 shows a single set of well-dispersed intense peaks,
characteristic of a folded protein in solution that undergoes limited
chemical exchange on the ms time scale (Figure C).The only available structure of
mβ2m is the crystal structure of the protein bound
to the heavy chain of the major histocompatibility complex (MHC-I).[38] In the case of hβ2m, binding
to the heavy chain causes conformational changes particularly in the
AB loop and the D strand of the protein.[39] To determine whether the crystal structure of mβ2m bound to the MHC-I complex constitutes a good representation for
the structure of the monomeric protein in solution, residual dipolar
couplings (RDC) were measured. Figure D shows that there is excellent agreement (R2 = 0.85) between the measured RDCs and those
back-calculated from the crystal structure of MHC-I-bound mβ2m (Figure D), confirming the identity of the solution structure of monomeric
mβ2m with that bound to MHC-I. Therefore, differences
in the structures of the native proteins cannot explain the different
amyloid potential of the two variants.We next assessed whether
differences in thermodynamic and/or kinetic
stability between mβ2m and hβ2m/ΔN6
could rationalize their different amyloid propensity. Equilibrium
denaturation experiments revealed that mβ2m is less
stable than hβ2m (ΔΔG°un = −12.4 kJ/mol) (Figure A, 2B and Supplementary Table 1). Remarkably, mβ2m is less stable than the aggregation prone ΔN6 (Figure A, 2B) demonstrating that thermodynamic instability cannot explain
the inability of mβ2m to form amyloid. Notably, ΔN6
shows a reduced m-value compared with hβ2m and mβ2m, consistent with exposure of hydrophobic residues that are
normally buried in the core of hβ2m (10 of the 17
core residues become more exposed in ΔN6[28]). Hydrogen exchange experiments monitored by 1H–15N HSQC spectra revealed that mβ2m is also kinetically less stable than hβ2m, with
amide protons exchanging with the solvent more rapidly than hβ2m, while ΔN6 is the least kinetically stable of the
three proteins studied here (Figure C, Figure S1A–C, and Figure S2). NMR relaxation experiments on native mβ2m also showed no regions of increased dynamics on the ps–ns
time scale, apart from the DE loop which is known to be flexible in
all β2m variants (Figure S2D–F). Thus, there is no correlation between thermodynamic or kinetic
stability and amyloidogenicity of these different β2m variants.
Figure 2
Thermodynamic and kinetic stability do not correlate with
amyloid
propensity. (A) Equilibrium denaturation curves for mβ2m, hβ2m, and ΔN6 monitored using tryptophan
fluorescence (75 mM sodium phosphate buffer pH 6.2, 25 °C). (B)
Unfolding free energies obtained by fitting data in (A) to a two state
model (see Table S1). (C) Representative
hydrogen exchange profiles for the amide hydrogen of residue 83 in
hβ2m, mβ2m, and ΔN6 at 25
°C and pH 6.2 (see Figure S2).
Thermodynamic and kinetic stability do not correlate with
amyloid
propensity. (A) Equilibrium denaturation curves for mβ2m, hβ2m, and ΔN6 monitored using tryptophan
fluorescence (75 mM sodium phosphate buffer pH 6.2, 25 °C). (B)
Unfolding free energies obtained by fitting data in (A) to a two state
model (see Table S1). (C) Representative
hydrogen exchange profiles for the amide hydrogen of residue 83 in
hβ2m, mβ2m, and ΔN6 at 25
°C and pH 6.2 (see Figure S2).
Real-Time Characterization
of a Transient Folding Intermediate
We next investigated
whether the folding pathway of mβ2m also involves
transient formation of an intermediate containing trans X-Pro 32 (known as the IT state[28]), the accumulation of which has been shown to
correlate directly with the rate of amyloid formation of the human
protein.[9] For these experiments, mβ2m was unfolded either by incubating the protein at pH 2.0
or by the addition of 8 M urea at pH 6.2. Refolding was then initiated
by dilution to a buffer of pH 7.2 or to a buffer lacking urea (see Methods, Figure S3),
and NMR spectra were collected in real time to track the refolding
reaction in residue-specific detail. In the case of hβ2m, and in accordance with previous studies,[28] a well-dispersed spectrum was observed 3 min after refolding was
initiated, in which only small chemical shift differences are detected
in comparison with those of the native protein (Figure A and 3B). These results
indicate that a native-like intermediate (the IT state)
accumulates during folding of hβ2m, consistent with
previous results.[9,28]
Figure 3
Folding of hβ2m and mβ2m in real-time.
(A) 1H–15N SOFAST HSQC spectrum of native
hβ2m in 10 mM sodium phosphate pH 6.2. (B) The 1H–15N SOFAST HSQC spectrum of hβ2m collected 3 min after refolding was initiated by urea dilution.
Peaks that are already in their native positions are colored gray,
while peaks with non-native chemical shifts are shown in red. (C)
The 1H–15N HSQC spectrum of ΔN6
closely resembles the spectrum of the real-time folding intermediate
of hβ2m. An overlay of the spectra shown in B and
C is shown as an inset. (D) 1H–15N HSQC
spectrum of native mβ2m in 10 mM sodium phosphate
pH 6.2. (E) The 1H–15N BEST-TROSY-HSQC
of mβ2m collected 3 min after refolding was initiated
by urea dilution. Peaks that are already in their native positions
are colored green while peaks with non-native chemical shifts are
shown in purple. (F) The 1H–15N HSQC
spectrum of mβ2m at pH 3.6 closely resembles the
spectrum of the real-time folding intermediate of mβ2m.
Folding of hβ2m and mβ2m in real-time.
(A) 1H–15N SOFAST HSQC spectrum of native
hβ2m in 10 mM sodium phosphate pH 6.2. (B) The 1H–15N SOFAST HSQC spectrum of hβ2m collected 3 min after refolding was initiated by urea dilution.
Peaks that are already in their native positions are colored gray,
while peaks with non-native chemical shifts are shown in red. (C)
The 1H–15N HSQC spectrum of ΔN6
closely resembles the spectrum of the real-time folding intermediate
of hβ2m. An overlay of the spectra shown in B and
C is shown as an inset. (D) 1H–15N HSQC
spectrum of native mβ2m in 10 mM sodium phosphate
pH 6.2. (E) The 1H–15N BEST-TROSY-HSQC
of mβ2m collected 3 min after refolding was initiated
by urea dilution. Peaks that are already in their native positions
are colored green while peaks with non-native chemical shifts are
shown in purple. (F) The 1H–15N HSQC
spectrum of mβ2m at pH 3.6 closely resembles the
spectrum of the real-time folding intermediate of mβ2m.As previously reported, the spectrum
of ΔN6 is very similar
to that of the human IT state (Figure C).[28] In marked
contrast with the behavior of hβ2m, however, the 1H–15N HSQC spectrum of mβ2m 3 min after refolding is initiated revealed only ∼20 intense
peaks with limited chemical shift dispersion in the 1H
dimension which coexist with the most intense peaks of the native
state (Figure D and 3E). Interestingly, the partially folded state of
mβ2m at pH 3.6 gives rise to a 1H–15N HSQC spectrum that closely resembles the spectrum collected
at pH ≈ 6.2, 3 min after refolding was initiated (Figure F). These results
suggest that partially folded species are significantly populated
during the folding of mβ2m, but that these species
differ in structure and/or dynamics compared with their human counterparts.In order to assign the real-time spectrum of the intermediate state
of mβ2m, continuous, NUS NMR spectra (2D-BEST-TROSY
HSQC, 3D-HNCA+, and 3D-HNCO+) were collected during refolding and
the whole data set was coprocessed together, resulting in a temporal
resolution of a few minutes.[36] Importantly,
and in contrast with other real-time studies of protein folding which
consist of acquisition of sequential stand-alone spectra,[40] this NUS approach requires the acquisition of
only a single spectrum. Therefore, it does not require prior knowledge
about the folding reaction in order to decide on the length of each
individual experiment, since the time resolution can be determined
in the processing step. Additionally, increased sensitivity is achieved
by coprocessing less sensitive 3D NMR spectra (e.g., HNCA) with 2D
experiments (e.g., HSQC).[41]The same
set of intense resonances shown in Figure E were observed in 3D real-time spectra,
consistent with these residues being flexible in the folding intermediate
of mβ2m. As only 20 spin systems are present in the
real-time HNCA spectrum, assignment was challenging. To overcome this
issue, further backbone assignment experiments were performed on mβ2m at pH 3.6 (Figure F) and mβ2m at pH 6.2 with 1 M urea added,
both of which gave rise to spectra similar to those of the kinetic
intermediate (Figure F and data not shown), removing the need for rapid data acquisition
(see Methods). The residue-type specific information
of the Cβ atoms from these equilibrium experiments greatly facilitated
the assignment of the real-time HNCA spectrum.The assignment
walk on the Cα resonances of mβ2m 5 min after
folding was initiated is shown in Figure A. The assignment revealed
that all of the intense peaks shown in Figure E correspond to residues located in the N-terminal
region, the A strand, and the AB loop of mβ2m (Figure B and 4C), regions of the polypeptide chain whose dynamics have been
implicated in the initiation of the aggregation of the human protein.[19,28] The C-terminal four residues of the protein were also detected with
chemical shifts that are different (ΔδH+N >
2 ppm) from those in the native structure. The backbone assignments
(N, NH, Cα, Cβ, CO atoms; Supplementary Table 2) allow the accurate prediction of the order parameter
S2 and, therefore, an assessment of protein dynamics. Figure B and 4C show that the 20 N-terminal residues show significantly
increased dynamics in the folding intermediate in comparison with
the native state, while the C-terminal four residues, while visible,
have conformational dynamics similar to those of the native protein.
Figure 4
The early
folding intermediate of mβ2m. (A) The
assignment walk on the Cα atoms of the real-time BEST-HNCA spectrum
of mβ2m collected 5 min after refolding was initiated
by urea dilution at pH 6.2. (B) Predicted S2 parameters
for the folding intermediate of mβ2m. The intense
peaks shown in Figure E are shown in dark blue. The S2 parameters of the native
state are shown as light blue bars and as a red line. (C) Residues
observed in the real-time spectrum of the folding intermediate are
highlighted in red in the structure of mβ2m. Pro
32 is shown as yellow spheres. (D) Far-UV CD spectra of native mβ2m at pH 6.2 (green) and of the folding intermediate 3 min
after folding was initiated by a pH jump from pH 2.0 to pH 6.2 (red).
(E) Normalized fluorescence signal at the end of each stopped-flow
transient (20 s) as a function of urea concentration for mβ2m in the absence (red) or presence (black) of 0.4 M sodium
sulfate. The data were fitted globally to a two-state model (see Methods).
The early
folding intermediate of mβ2m. (A) The
assignment walk on the Cα atoms of the real-time BEST-HNCA spectrum
of mβ2m collected 5 min after refolding was initiated
by urea dilution at pH 6.2. (B) Predicted S2 parameters
for the folding intermediate of mβ2m. The intense
peaks shown in Figure E are shown in dark blue. The S2 parameters of the native
state are shown as light blue bars and as a red line. (C) Residues
observed in the real-time spectrum of the folding intermediate are
highlighted in red in the structure of mβ2m. Pro
32 is shown as yellow spheres. (D) Far-UV CD spectra of native mβ2m at pH 6.2 (green) and of the folding intermediate 3 min
after folding was initiated by a pH jump from pH 2.0 to pH 6.2 (red).
(E) Normalized fluorescence signal at the end of each stopped-flow
transient (20 s) as a function of urea concentration for mβ2m in the absence (red) or presence (black) of 0.4 M sodium
sulfate. The data were fitted globally to a two-state model (see Methods).The molten-globule-like behavior of the intermediate state
(named
here I1) prevents the direct observation of the majority
of the resonances (apart from the 20 most flexible) in 1H-detected experiments, as they are in conformational/solvent exchange.
To overcome this problem direct 13C-detection experiments
were performed on mβ2m at pH 3.6 in order to obtain
information about the structural properties of the rest of the protein
in the I1 state. These experiments revealed ∼80
resonances, 20 of which have sharp lines which correspond to the 20
N-terminal residues assigned above. Other resonances show broader
lines suggesting that they correspond to residues with a higher degree
of folding (Figure S5). The far-UV CD spectrum
of mβ2m obtained 3 min after the pH jump from pH
2.0 to pH 6.2 shows that in I1 73% of native β-sheet
structure is already formed, as quantified by the ratio of the intensities
at 219 nm (Figure D). These results show that mβ2m at pH 3.6 is partially
structured, with the majority of residues being in a β-sheet
conformation, potentially native-like. These residues undergo chemical
exchange on the ms time scale (or exchange rapidly with solvent) and,
therefore, cannot be observed in the 1H–15N spectrum shown in Figure E.In order to estimate the stability of the I1 state,
stopped-flow fluorescence experiments were used to determine the fluorescence
intensity of mβ2m 20 s after folding was initiated
(Figure E). These
experiments revealed that, by contrast with the IT state
of hβ2m for which the ΔG°un is −9.57 ± 0.54 kJ/mol at 37 °C,[9] the I1 state of mβ2m (ΔG°un = ∼ –4.8
kJ/mol at 37 °C) is only marginally stable in solution, in accordance
with the real-time NMR data (Figure E). Overall, the data show that mβ2m folds through a flexible/molten globule-like intermediate state
in which the N-terminus and the A strand are dynamic and detached
from a native-like β-sandwich fold (I1) (Figure C).
The flexible
intermediate I1 is not aggregation-prone
The amyloid
fibrils of hβ2m are composed of parallel
in register β-strands,[42,43] while in the native
monomer the β-strands are all antiparallel (Figure A). Thus, a major conformational
change has to occur on the pathway to fibrils. Detachment of the A
strand might represent a first step toward the remodeling of the native
protein, and therefore, the early intermediate of mβ2m, I1, might be expected to be highly amyloidogenic. To
test this hypothesis, aggregation assays were performed using ΔN6
at pH 6.2 as a mimic of the highly aggregation-prone state IT, and mβ2m at pH 3.6, conditions which favor the
less structured intermediate state (I1) of mβ2m. Consistent with previous results, these experiments showed
that ΔN6 aggregates rapidly at pH 6.2 with a lag time of ∼30
h, resulting in the formation of amyloid fibrils (Figure A). In marked contrast, no
increase in ThT fluorescence was observed for mβ2m at pH 3.6 (Figure A). Indeed, the majority of the murine protein remained soluble after
100 h of incubation, while ΔN6 was quantitatively converted
into amyloid fibrils (Figure B and 5C). Interestingly, the small
amount of mβ2m that was not found in the supernatant
also formed short fibrils ∼300 nm in length (Figure C). These results show that
the partially folded state of mβ2m is not highly
aggregation prone. On the other hand, the specific structural features
of the native-like IT intermediate of hβ2m are crucial for assembly.
Figure 5
Amyloidogenicity of intermediate states of mβ2m and hβ2m. (A) ThT fluorescence assays of
60 μM
ΔN6 in 10 mM sodium phosphate buffer pH 6.2 (red) or 60 μM
mβ2m in 10 mM sodium phosphate, 10 mM sodium acetate
pH 3.6 (green). Five replicates are shown for each protein. (B) SDS-PAGE
gel of the end points shown in (A). 20 μL of the reaction were
spun down using a benchtop centrifuge for 20 min and a sample of the
total reaction (W) or of the supernatant (S/N) after centrifugation,
was analyzed by SDS-PAGE. (C) AFM image of 60 μM mβ2m after 95 h of incubation (green in A, note that fibrils
correspond to <5% of the protein added) and electron micrograph
of 60 μM ΔN6 (fibrils correspond to >95% of the protein
added) after 95 h of incubation (red in A). Scale bar represents 500
nm.
Amyloidogenicity of intermediate states of mβ2m and hβ2m. (A) ThT fluorescence assays of
60 μM
ΔN6 in 10 mM sodium phosphate buffer pH 6.2 (red) or 60 μM
mβ2m in 10 mM sodium phosphate, 10 mM sodium acetate
pH 3.6 (green). Five replicates are shown for each protein. (B) SDS-PAGE
gel of the end points shown in (A). 20 μL of the reaction were
spun down using a benchtop centrifuge for 20 min and a sample of the
total reaction (W) or of the supernatant (S/N) after centrifugation,
was analyzed by SDS-PAGE. (C) AFM image of 60 μM mβ2m after 95 h of incubation (green in A, note that fibrils
correspond to <5% of the protein added) and electron micrograph
of 60 μM ΔN6 (fibrils correspond to >95% of the protein
added) after 95 h of incubation (red in A). Scale bar represents 500
nm.
A native-like IT intermediate is populated on the
pathway to native mβ2m
The data presented
above demonstrate that the conformational properties of the dynamic
I1 state of mβ2m are different from those
the native-like hβ2m IT state. However,
additional states could be populated after the formation of I1 and prior to the formation of native mβ2m. Indeed, as the folding time progresses a third set of peaks (apart
from the native and the flexible intermediate states (Figure )) emerges in the real-time 1H–15N HSQC spectrum (Figure S4). These peaks show small chemical shift differences
compared with the native mβ2m resonances and are
generally broad (Figure S4) suggesting
that additional, more native-like states are populated at later times
during the folding of the protein. This observation presumably reflects
an ordered assembly mechanism, in which the initially highly dynamic
intermediate (I1) folds to the native state via a transiently
populated more structured (IT-like) state.To investigate
this possibility further, partially folded mβ2m at
pH 3.6 (which mimics the I1 state – Figures E and 3F) was allowed to fold by a rapid pH jump to pH 6.2 and folding was
monitored in real time using NMR. The 1H–15N HSQC spectrum collected 3 min after refolding was initiated showed
a well dispersed spectrum (Figure A) in striking and marked contrast with the molten
globule-like spectrum of the I1 state shown in Figure E. Indeed, the spectrum
obtained 3 min after the pH jump is reminiscent of that of native
mβ2m with significant chemical shift differences
being limited to residues in the N-terminal region (residues 1–6),
the BC, DE, and FG loops (Figure A and 6B). Moreover, the peaks
that show chemical shift differences from the native protein are remarkably
similar to the third set of peaks observed in Figure S4B, consistent with folding from the partially folded
state (I1) to a more native-like intermediate (presumably
IT). Importantly, residues that show significant chemical
shift changes are surrounded by residues whose resonances are not
detected in the real-time NMR spectrum (Figure B). These areas reside in close spatial proximity
to Pro 32 in the native structure and, therefore, are exchange-broadened.
A similar scenario has been observed for the real-time folding intermediate
of hβ2m (IT).[40] Furthermore, ΔN6 shows chemical shift differences to native
hβ2m in these same regions.[28] Together, the results show that mβ2m folds through
a native-like intermediate state that has similar structural properties
to the amyloidogenic IT state of hβ2m.
However, due to its decreased stability, this species is copopulated
with an ensemble of partially folded, flexible states in which the
N-terminal region is highly disordered (I1).
Figure 6
Detection of
a native-like folding intermediate for mβ2m. (A)
The 1H–15N SOFAST HSQC
spectrum of mβ2m collected 3 min after refolding
was initiated from the partially folded state at pH 3.6 (blue), overlaid
with the 1H–15N SOFAST HSQC of native
mβ2m (collected after 90 min) (gray). Peaks corresponding
to the molten globule I1 state are colored in pink. (B)
Per residue combined 1H–15N chemical
shift differences between the native and the IT state of
mβ2m, using the spectra displayed in (A). Blue dots
represent residues for which assignments are missing in the native
spectrum. Residues that show chemical shift differences greater than
1 ppm (dashed line) are colored yellow, those that show chemical shift
differences less than 1 ppm are shown in gray, and residues that are
broadened beyond detection in the 3 min spectrum are colored red.
The strucure of mβ2m colored in the same color scheme
is shown on the right.
Detection of
a native-like folding intermediate for mβ2m. (A)
The 1H–15N SOFAST HSQC
spectrum of mβ2m collected 3 min after refolding
was initiated from the partially folded state at pH 3.6 (blue), overlaid
with the 1H–15N SOFAST HSQC of native
mβ2m (collected after 90 min) (gray). Peaks corresponding
to the molten globule I1 state are colored in pink. (B)
Per residue combined 1H–15N chemical
shift differences between the native and the IT state of
mβ2m, using the spectra displayed in (A). Blue dots
represent residues for which assignments are missing in the native
spectrum. Residues that show chemical shift differences greater than
1 ppm (dashed line) are colored yellow, those that show chemical shift
differences less than 1 ppm are shown in gray, and residues that are
broadened beyond detection in the 3 min spectrum are colored red.
The strucure of mβ2m colored in the same color scheme
is shown on the right.
Discussion
Characterization of Protein Energy Landscapes
Using Sparse Data
The results presented above highlight the
importance of determining
the precise details of the folding energy landscape of a protein in
order to elucidate whether one or more partially folded, or non-native
states, have the potential to initiate amyloid assembly. Characterization
of ensembles of interconverting non-native species that not only are
lowly populated but also have a short lifetime, such as those involved
in protein folding and aggregation, is a challenging task, even for
the most advanced biophysical methods. While time-resolved NMR studies
on proteins can be highly informative, these studies usually suffer
from low resolution and poor sensitivity. By combining the use of
sparsely sampled NMR and coprocessing of more complicated/less sensitive
experiments with others that show increased sensitivity, we demonstrate
here the detection and atomic level depiction of the early molten
globule state, I1, of mβ2m, that is populated
for only ∼15 min, a task that would not have been possible
using standard NMR methodologies (see Supplementary Methods). The power of the real-time NMR experiments allowed
us to identify conditions that stabilize the I1 state (pH
3.6 or addition of 1 M urea at pH 6.2) and to perform more detailed
NMR experiments on the trapped intermediate state that led to a complete
description of the folding mechanism of the murine protein. The approach
is potentially applicable to other amyloidogenic proteins or proteins
that fold through the accumulation of transient intermediate states.
The precise balance between folding intermediates determines
the aggregation propensity of β2m
The folding
pathway of hβ2m has been investigated in detail over
the past decade using different protein variants and different techniques.[9,28,44−48] Together, these studies have shown that the folding
of hβ2m involves the formation of a native-like intermediate
IT that is kinetically trapped by virtue of the non-native trans X-Pro 32 bond.[9,47] This species is preceded
by a less well characterized species (I1)[44] that forms in the dead time of a stopped flow experiment
(<3 ms) and is less structured than the IT state (Figure ). The fine details
of the exchange processes between these different folding intermediates
has a dramatic effect on the propensity to aggregate. For hβ2m the structured aggregation-prone IT state is
the most highly populated species during folding, accumulating, on
average, to ∼4% (pH 7.0, 37 °C) at equilibrium.[9,10] By contrast, the flexible I1 state represents the most
highly populated intermediate state during the folding of mβ2m. Indeed, the most intense peaks of the I1 state
(but not those of the IT state) are visible in the spectrum
of native mβ2m, enabling estimation of its equilibrium
concentration to ∼7% (Figure S6).
This reduces the population of the mβ2m IT state, with the effect that aggregation no longer occurs (at least
on an experimentally tractable timescale) (Figure ). Thus, although the folding mechanisms
of human and murine β2m are conserved (the same species
are populated on the pathway to the native state), the precise balance
between these states reduces the population of the key amyloidogenic
precursor IT for mβ2m and thus defines
the course of amyloid formation.
Figure 7
Balance between protein folding and aggregation.
The native-like
IT state is predominantly populated during the folding
of hβ2m (gray scheme, left). This allows the entrance
to the aggregation landscape (red scheme) as IT shows enhanced
amyloidogenicity. In the case of mβ2m (right) IT represents only a minor conformation during folding, but
instead the flexible molten globule-like state in which the A strand
is detached from the β-sandwich fold is the major non-native
species. As I1 is not aggregation-prone, mβ2m is protected from misfolding and instead folds to the native state
(the energy levels of the aggergation landscape are drawn for illustration
purposes only).
Balance between protein folding and aggregation.
The native-like
IT state is predominantly populated during the folding
of hβ2m (gray scheme, left). This allows the entrance
to the aggregation landscape (red scheme) as IT shows enhanced
amyloidogenicity. In the case of mβ2m (right) IT represents only a minor conformation during folding, but
instead the flexible molten globule-like state in which the A strand
is detached from the β-sandwich fold is the major non-native
species. As I1 is not aggregation-prone, mβ2m is protected from misfolding and instead folds to the native state
(the energy levels of the aggergation landscape are drawn for illustration
purposes only).Interestingly, urea denaturation
experiments on a partially folded
state of hβ2m formed at pH 3.6 have shown that the
N-terminal six residues and the A strand are the least stable regions,
while the rest of the protein forms a stable core.[49] These results are consistent with the real-time NMR studies
on the I1 state of mβ2m presented here,
showing that the conformational properties of the early partially
folded states of hβ2m and mβ2m are
similar. Interestingly, neither of these states is able to form long,
straight fibrils characteristic of amyloid, but instead they form
short rod-like fibrils (mβ2m at pH 3.6) or worm-like
fibrils (hβ2m at pH 3.6)[50] (Figure ).A direct link between decreased native state stability and increased
aggregation propensity has been observed for several proteins including
lysozyme,[51] transthyretin,[6] and antibody light chains.[52] Accordingly, destabilizing mutations enhance the rate of exchange
between the native protein and partially folded non-native species,
which show increased amyloidogenicity compared with the native state.
Interestingly, mβ2m is less thermodynamically and
kinetically stable than hβ2m and, as a consequence,
the molten globule-like nonamyloidogenic I1 state is the
most abundant non-native species (Figure ). The increased conformational dynamics
results in a protein that is unstable yet protected from amyloid assembly,
since I1 is not able to form amyloid. These findings argue
against a simple link between native state stability and amyloidogenicity
(at least for β2m). Instead, they highlight the importance
of the precise conformational properties of the native-like IT state that are vital for assembly.Together, the results
demonstrate that amyloid formation of β2m at neutral
pH is initiated via the highly structured IT state. Hence,
from the myriad of potential non-native conformations
that could be populated during folding, only the IT state
allows the entrance of β2m to the aggregation landscape
(Figure ). Such a
finding highlights the ordered specificity in the early stages of
assembly into amyloid and opens the opportunity to target a specific
non-native state in order to control the onset of aggregation, for
example through the development of antibodies, nanobodies, or small
molecules that specifically recognize this species. The results highlight
the importance of considering multiple factors in order to predict
amyloid formation. Hydrophobicity, the propensity of the sequence
to aggregate, the stability of the native state, solubility, transient
exposure of aggregation-prone regions through protein dynamics, and
the stability of the polypeptide sequence within the fully assembled
fibril structure itself, may all contribute to enhanced amyloidogenicity.
Although, these factors are well understood individually, the interplay
between them during aggregation remains poorly explained. The results
presented emphasize the importance of understanding the energy landscape
of aggregation in intricate detail, from both thermodynamic and kinetic
view points, in order to predict whether or not a protein will aggregate
and how/why minor alterations in solution conditions/amino acid sequence
can have a dramatic effect on the course of assembly, by small changes
in the relative populations of amyloidogenic versus nonamyloidogenic
states.
Conclusion
In this study we have
used NUS NMR methods to study the relationship
between protein folding and aggregation of a globular protein that
forms amyloid fibrils from a structured precursor state, using β2m as the test protein. We show that the least thermodynamically
stable protein is the least aggregation-prone sequence of the family
of proteins studied here. Analysis of the folding energy landscape
of the protein using real-time NMR revealed that the decreased stability
and decreased lifetime of a precise and well-defined native-like amyloidogenic
precursor (IT) are sufficient to tip the balance from aggregation
to folding. The power of sparsely sampled NMR allowed us not only
to detect a dynamic intermediate state (I1) of mβ2m but also to structurally characterize this species in residue-specific
detail. The results reveal that the least stable protein (mβ2m) populates predominantly a flexible intermediate (I1) that is not aggregation-prone, while its more stable counterpart
(hβ2m) folds through a native-like intermediate that
has enhanced amyloidogenicity. Subtle changes in the folding energy
landscape thus lead to dramatic changes in the aggregation outcome.
The results reveal that protein stability does not correlate with
aggregation propensity. Instead it is the precise balance and kinetic
partitioning of intermediate states that determines whether β2m will fold to the native state or aggregate to form amyloid
fibrils.
Authors: Enrico Rennella; Thomas Cutuil; Paul Schanda; Isabel Ayala; Vincent Forge; Bernhard Brutscher Journal: J Am Chem Soc Date: 2012-05-07 Impact factor: 15.419
Authors: E Rennella; T Cutuil; P Schanda; I Ayala; F Gabel; V Forge; A Corazza; G Esposito; B Brutscher Journal: J Mol Biol Date: 2013-05-03 Impact factor: 5.469
Authors: Andrew J Baldwin; Tuomas P J Knowles; Gian Gaetano Tartaglia; Anthony W Fitzpatrick; Glyn L Devlin; Sarah Lucy Shammas; Christopher A Waudby; Maria F Mossuto; Sarah Meehan; Sally L Gras; John Christodoulou; Spencer J Anthony-Cahill; Paul D Barker; Michele Vendruscolo; Christopher M Dobson Journal: J Am Chem Soc Date: 2011-08-19 Impact factor: 15.419
Authors: Magdalena I Ivanova; Michael R Sawaya; Mari Gingery; Antoine Attinger; David Eisenberg Journal: Proc Natl Acad Sci U S A Date: 2004-07-12 Impact factor: 11.205
Authors: Markus G Rudolph; Lucy Q Shen; Stephen A Lamontagne; John G Luz; Joseph R Delaney; Qing Ge; Bryan K Cho; Deborah Palliser; Carol A McKinley; Jianzhu Chen; Ian A Wilson; Herman N Eisen Journal: J Immunol Date: 2004-03-01 Impact factor: 5.422
Authors: Neil M Kad; Sarah L Myers; David P Smith; D Alastair Smith; Sheena E Radford; Neil H Thomson Journal: J Mol Biol Date: 2003-07-18 Impact factor: 5.469
Authors: Theodoros K Karamanos; Arnout P Kalverda; Gary S Thompson; Sheena E Radford Journal: Prog Nucl Magn Reson Spectrosc Date: 2015-05-27 Impact factor: 9.795
Authors: Theodoros K Karamanos; Matthew P Jackson; Antonio N Calabrese; Sophia C Goodchild; Emma E Cawood; Gary S Thompson; Arnout P Kalverda; Eric W Hewitt; Sheena E Radford Journal: Elife Date: 2019-09-25 Impact factor: 8.140
Authors: Samuel Lenton; Marco Grimaldo; Felix Roosen-Runge; Frank Schreiber; Tommy Nylander; Roger Clegg; Carl Holt; Michael Härtlein; Victoria García Sakai; Tilo Seydel; Susana C Marujo Teixeira Journal: Biophys J Date: 2017-04-25 Impact factor: 4.033
Authors: Murilo M Pedrote; Guilherme A P de Oliveira; Adriani L Felix; Michelle F Mota; Mayra de A Marques; Iaci N Soares; Anwar Iqbal; Douglas R Norberto; Andre M O Gomes; Enrico Gratton; Elio A Cino; Jerson L Silva Journal: J Biol Chem Date: 2018-05-31 Impact factor: 5.157
Authors: Hugh I Smith; Nicolas Guthertz; Emma E Cawood; Roberto Maya-Martinez; Alexander L Breeze; Sheena E Radford Journal: J Biol Chem Date: 2020-07-13 Impact factor: 5.157